JP5413788B2 - Liquid crystal display - Google Patents

Description

  The present invention relates to a liquid crystal display device, and more particularly to a transflective liquid crystal display device having a transmissive region and a reflective region.

  Liquid crystal display devices are largely classified into a passive matrix type and an active matrix type depending on a driving method.

  In the active matrix type, an active element such as a transistor or a diode is installed for each pixel, and these are sequentially selected in a time-division manner and turned on to charge a signal voltage to a capacitor formed for each pixel, and turned off. In this period, display is performed by holding the signal voltage. Compared with the passive matrix type in which voltage is applied to the liquid crystal by time-division matrix driving, display is possible with high contrast and large capacity display. Have.

  As an operation mode of the liquid crystal of the active matrix liquid crystal display device, the direction of the molecular axis of liquid crystal molecules (hereinafter referred to as a director) is rotated between the upper and lower substrates by approximately 90 degrees between the substrates, and the liquid crystal molecules are twisted. Conventionally, a twisted nematic (TN) mode in which display is performed by rotating a director in a vertical direction by an electric field perpendicular to the substrate has been used.

  However, this TN mode has a problem that the viewing angle is narrow. Therefore, in mobile applications that can be viewed from various directions, if the display from an oblique direction becomes invisible or if the large-capacity display advances and the screen area increases, the screen center is It looks different at the edges of the screen, making correct display impossible.

  To solve this problem, in-plane switching (IPS) mode or fringe field switching (FFS), in which an electric field is generated in a direction parallel to the substrate and the director is rotated in a horizontal plane, is displayed. ) Mode has been developed. In such a liquid crystal display device in which the liquid crystal is driven by an electric field parallel to the substrate, since the liquid crystal is aligned in the horizontal direction, the birefringence of the liquid crystal does not change greatly even if the viewpoint is moved. Compared with the device, a wide viewing angle can be achieved.

  Liquid crystal display devices are used as display screens for mobile phones, PDAs (Personal Digital Assistants), and business terminals because of their light weight, thinness, and low power consumption. Good display is possible, but there are scenes where visibility is greatly degraded due to the influence of outside light in the daytime outdoors or in bright offices, making it impossible to confirm the display. Therefore, a reflective liquid crystal display device capable of performing display by reflecting external light as a light source with a reflector, and a transflective liquid crystal capable of performing both displays by dividing a pixel into a reflective region and a transmissive region. Display devices have been developed (for example, see the following Patent Documents 1 to 3 regarding a transflective liquid crystal display device of a horizontal electric field type).

JP 2007-41572 A JP 2007-322941 A Japanese Patent Laid-Open No. 11-174491

  The liquid crystal display device of Patent Document 1 is a transflective liquid crystal display device having a transmissive region and a reflective region in a pixel using the IPS mode. The structure is shown in FIGS. FIG. 26 is a plan view showing the structure of a transflective liquid crystal display device, where (a) is a structure excluding a reflector, (b) is a structure with a reflector added, and (c) is a black matrix. The structure with added is shown. 27 is a cross-sectional view showing the structure of the transflective liquid crystal display device, in which FIG. 27A is a cross-sectional view taken along line AA ′ in FIG. 26C, FIG. 27B is a cross-sectional view taken along line BB ′, and FIG. ) Shows the structure of the CC ′ cross section. FIG. 28 is a diagram schematically illustrating the configuration of wiring and electrodes of one pixel, and FIG. 29 is a diagram illustrating waveforms of a transmission common signal and a reflection common signal.

  As shown in FIGS. 26 to 29, the liquid crystal display device of Patent Document 1 is arranged in a matrix on a transparent insulating substrate (hereinafter referred to as a TFT substrate 10) in which thin film transistors (TFTs) exist. A plurality of scanning lines 12, signal lines (data lines 13), and a common electrode line. The common electrode line is a transmissive common electrode line 18 a that applies a reference potential to the transmissive region 3, and a reflective common that applies a reference potential to the reflective region 2. The electrode line 18b includes a transmission TFT 14a and a transmission pixel electrode 17a corresponding to the transmission region 3 of the pixel at the intersection of the scanning line 12 and the data line 13, and a reflection corresponding to the reflection region 2 of the pixel. A TFT 14b and a reflective pixel electrode 17b are provided.

  A transmissive common electrode 18a 'is electrically connected to the transmissive common electrode line 18a, and a reflective common electrode 18b' is electrically connected to the reflective common electrode line 18b.

  The transmissive pixel electrode 17a and the transmissive common electrode 18a 'are installed in a stripe shape so that both electrodes are parallel to each other, and can generate an electric field (transmission) mainly composed of components orthogonal to both the electrodes parallel to the substrate surface. The reflective pixel electrode 17b and the reflective common electrode 18b ′ are arranged in a stripe shape so that both electrodes are parallel to each other, and an electric field (reflection) mainly composed of a component orthogonal to both electrodes parallel to the substrate surface. Can be generated.

  In the reflective region 2, a reflective plate 16 is disposed below the reflective pixel electrode 17a and the reflective common electrode 18b 'via an insulating film 15b.

  According to Patent Document 1, in a transflective liquid crystal display device using an IPS mode, the transmissive region 3 is normally black display that is black when no voltage is applied and white when a voltage is applied, and the reflective region 2 is white when no voltage is applied. Since normally white display becomes black when a voltage is applied, the transmission common signal and the reflection common signal need to be inverted in phase as shown in FIG. 29 when the same video signal is used.

  In that case, different potentials are applied between adjacent pixels or between a transmissive region and a reflective region in a pixel, so that an electric field unrelated to display is generated between the pixels. Therefore, in order to prevent such light leakage, a liquid crystal display device generally has a structure in which light is shielded by a black matrix 22 made of a metal such as chromium, an oxide laminated film thereof, or a resin in which carbon particles are dispersed. Used.

  Here, in the case of the TN mode active matrix liquid crystal display device, the black matrix 22 on the counter substrate 20 is shielded from the electric field by the transparent electrode formed on the liquid crystal surface side of the counter substrate 20. An electric field that affects the display is not generated at any potential.

  However, in the case of an IPS mode active matrix liquid crystal display device, the black matrix 22 does not have a shielding electrode such as a TN mode transparent electrode between the black matrix 22 and the potential of the black matrix 22 is the TFT substrate 10. Because it is affected by the electrical signal applied to the display, it may affect the display.

  In particular, in the IPS mode transflective liquid crystal display device, as shown in FIG. 27, the transmissive common electrode 18a ′ and the reflective common electrode 18b ′ are arranged so as to overlap the black matrix 22, respectively. As a result, a potential difference is generated between the black matrix 22 and the transmissive common electrode 18a ′ and the transmissive pixel electrode 17a. As a result, the director rotates in the plane direction, causing light leakage.

  In order to solve such a problem, a method of applying a potential to the black matrix 22 is disclosed in Patent Document 3.

  In Patent Document 3, by applying the same signal as the signal applied to the common electrode to the black matrix 22, the potential of the black matrix 22 is set to the same potential as that of the common electrode, and the influence on the director is suppressed by the potential difference.

  However, this document proposes a method of applying the same potential as that of the common electrode as a method for solving the influence of the potential at which the data line and the black matrix face each other in the transmissive IPS. In the inversion driving method described above, since there are two types of common signals, they cannot be matched to both, and cannot be solved.

  Further, in order to apply the potential in this way, it is necessary to use a low resistance metal such as chromium or an oxide laminated film thereof as the material of the black matrix 22, and these metal films are formed by the light incident from the backlight. However, there is a problem that light is leaked by being emitted after multiple reflection with the metal film, the scanning line 12, the data line 13, and the transmissive common electrode 18a '.

  Furthermore, in order to give a potential to the counter substrate side, there is a problem that a plurality of processes are added as described in Patent Document 3, and in recent years, ionic component liquid crystal from the color filter of the counter substrate is present. Since it is necessary to suppress elution to the black filter, an overcoat is further formed on the color filter, and in order to apply a potential to the black matrix, a process of opening a through hole in the overcoat is also required.

  The present invention has been made in view of the above-described problems, and its main purpose is to suppress light leakage caused by the potential generated between the electrode on the active matrix substrate and the black matrix on the counter substrate. It is an object of the present invention to provide a liquid crystal display device capable of achieving the above.

  In order to achieve the above object, the present invention is sandwiched between one substrate on which switching elements are arranged in a matrix, the other substrate on which a black matrix made of a conductive material is formed, and the two substrates. A liquid crystal display device comprising: a liquid crystal layer, wherein the liquid crystal display device includes a first region that is normally black display, and a second region that is normally white display, and the first region includes the first region. One substrate includes a first pixel electrode electrically connected to the switching element, a first common electrode, and a first common electrode line for supplying a first common signal to the first common electrode, A second pixel having a second common electrode on the one substrate or the other substrate in the second region and electrically connected to the switching element on the one substrate in the second region; Electrode and said second A second common electrode line for supplying a second common signal to the through electrode is provided, and a potential different from that of the second common electrode line is provided between the second common electrode line and the black matrix in the periphery of the display region. A conductive film supplied with is formed.

  According to the liquid crystal display device of the present invention, it is possible to suppress light leakage caused by the potential generated between the electrode on the active matrix substrate and the black matrix on the counter substrate.

  As shown in the background art, when the IPS mode is adopted in the transflective liquid crystal display device, the black display and the white display are reversed, and in the normal driving method, when the transmission region is normally black, There is a problem that the reflection area becomes normally white. First, this display inversion will be described.

  In the following description, the polarizing axes of the light emitting side (display surface side) polarizing plate (first polarizing plate) and the light incident side (backlight side) polarizing plate (second polarizing plate) are the same. Assume that they are arranged orthogonally. In the liquid crystal layer, it is assumed that the liquid crystal molecules are arranged so that the direction of the liquid crystal molecules is shifted by 90 ° from the direction of the polarization axis (light transmission axis) of the second polarizing plate when no voltage is applied. For example, if the polarization axis direction of the second polarizing plate is 0 °, the polarization axis direction of the first polarizing plate is set to 90 °, and the liquid crystal molecule major axis direction of the liquid crystal layer is set to 90 °. The cell gap of the liquid crystal layer is adjusted so that the retardation Δn · d (Δn is the refractive index anisotropy of liquid crystal molecules, d is the cell gap of the liquid crystal) is λ / 2 (λ is the wavelength of light) in the transmission region. In the reflection region, the cell gap is adjusted so that the retardation is λ / 4.

[Reflection area]
First, in the reflection region, when no voltage is applied to the liquid crystal layer, linearly polarized light in the 90 ° direction (longitudinal direction) that has passed through the first polarizing plate is incident on the liquid crystal layer. In the liquid crystal layer, since the optical axis direction of the incident linearly polarized light coincides with the major axis direction of the liquid crystal molecules, the 90 ° linearly polarized light passes through the liquid crystal layer as it is and enters the reflecting plate. The reflection plate reflects the light as 90 ° linearly polarized light, passes through the liquid crystal layer again, and enters the first polarizing plate. Since the polarization axis direction of the first polarizing plate is 90 °, the transmitted light passes through the first polarizing plate, and thus white display is performed.

  Similarly, when a voltage is applied to the liquid crystal layer, 90 ° direction (longitudinal) linearly polarized light that has passed through the first polarizing plate is incident on the liquid crystal layer. In the liquid crystal layer, the major axis direction of the liquid crystal layer changes from 0 ° to 45 ° in the substrate plane by voltage application, so that the polarization direction of incident light and the major axis direction of the liquid crystal molecules are shifted by 45 °. Since the retardation of the liquid crystal is set to λ / 4, the linearly polarized light enters the reflecting plate in a clockwise circular polarization state. The light reflected by the reflecting plate becomes a counterclockwise circularly polarized state, passes through the liquid crystal layer again, becomes linearly polarized light in the horizontal direction (0 ° direction), and enters the first polarizing plate. Since the polarization axis direction of the first polarizing plate is 90 °, the reflected light cannot be transmitted and black display is obtained. Therefore, it is normally white in the reflection region.

[Transparent area]
On the other hand, in the transmissive region, when no voltage is applied to the liquid crystal layer, laterally linearly polarized light that has passed through the second polarizing plate is incident on the liquid crystal layer. In the liquid crystal layer, the polarization direction of the incident light and the molecular major axis direction are orthogonal to each other, so that the liquid crystal layer passes through the liquid crystal layer without changing the polarization state and enters the first polarizing plate. . Since the polarization axis direction of the first polarizing plate is 90 °, the transmitted light cannot pass through the first polarizing plate, resulting in black display.

  Similarly, when a voltage is applied to the liquid crystal layer, the linearly polarized light in the horizontal direction that has passed through the second polarizing plate is incident on the liquid crystal layer. In the liquid crystal layer, the major axis direction of the liquid crystal layer changes from 0 ° to 45 ° in the substrate plane by applying a voltage, so that the polarization direction of light incident on the liquid crystal layer and the major axis direction of the liquid crystal molecules are shifted by 45 °. In addition, since the retardation of the liquid crystal is set to λ / 2, the linearly polarized light in the horizontal direction becomes the linearly polarized light in the vertical direction and enters the first polarizing plate. Since the polarization axis direction of the first polarizing plate is 90 °, the transmitted light passes through the first polarizing plate and becomes white display. Accordingly, the transmission region is normally black.

  As described above, the transflective liquid crystal display device has a problem that the white display and the black display are reversed in the reflective region and the transmissive region both when the electric field is applied to the liquid crystal layer and when the electric field is not applied. Therefore, in order to solve this problem, a method of applying a voltage to be inverted between the reflection region and the transmission region (for example, gate line inversion driving or dot inversion driving) is used.

  If this method is used, when a voltage is applied only to the transmissive region, both the transmissive region and the reflective region are displayed in white, and when a voltage is applied only to the reflective region, both the transmissive region and the reflective region are displayed in black. However, by applying different voltages to the reflective region and the transmissive region, a potential difference is generated between the black matrix and the wiring, and an electric field is generated. This electric field causes the director to rotate in the plane direction, thereby causing light leakage.

  That is, when a voltage having the same phase is applied to the reflective common electrode and the transmissive common electrode, the black matrix potential is in phase with the reflective common electrode and the transmissive common electrode, as shown in FIG. The potential difference between the electrode and the black matrix, and the potential difference between the transmissive common electrode and the black matrix are both small, but when a reverse-phase voltage is applied to the reflective common electrode and the transmissive common electrode, the black matrix potential is It is in phase with either one of the transmissive common electrodes (FIG. 30 (b) or (c)), or an intermediate potential between the common electrodes (FIG. 30 (d)). The potential difference and the potential difference between the transmissive common electrode and the black matrix increase, and the director rotates in the plane direction due to the electric field due to this potential difference.

  Here, the charges formed by the black matrix, each electrode, and the wiring are calculated.

First, regarding the display portion, as shown in FIG. 31, the scanning line potential is V _G , the data line potential is V _D , the transmissive common electrode potential is V _TC , the transmissive pixel electrode potential is V _TP , and the reflective common electrode. _RC of potential _V, potential _{V RP} of the reflective pixel electrodes, capacitance _{C BM-Ga} between the scanning line and the black matrix, capacity _{C BM-Da} between the data line and the black matrix, transparent common electrode and the black The capacitance between the matrix is C _BM-TCE , the capacitance between the transmissive pixel electrode and the black matrix is C _BM-TPE , the capacitance between the reflective common electrode and the black matrix is C _BM-RCE , and the reflective pixel electrode and the black matrix are When the capacitance between them is _CBM-RPE , the charge formed by the black matrix, each electrode, and the wiring is expressed by the following equation.

_{C BM-TCE × V TC +} C BM-TPE × V TP + C BM-RCE × V RC + C BM-RPE × V RP + C BM-Ga × V G + C BM-Da × V D ... (1)

Further, regarding the peripheral portion, as shown in FIG. 32, the scanning line potential is V _G , the data line potential is V _D , the transmission common electrode line potential is V _TCL , and the reflection common electrode line potential is V _RCL . The capacitance between the line and the black matrix is C _BM-Gb , the capacitance between the data line and the black matrix is C _BM-Db , the capacitance between the transmissive common electrode line and the black matrix is C _BM-TCL , and the reflective common electrode line Assuming that the capacitance between the black matrix and the black matrix is _CBM-RCL , the charge formed by the black matrix and each wiring is expressed by the following equation.

_{C BM-TCL × V TC +} C BM-RCL × V RC + C BM-Gb × V G + C BM-Db × V D ... (2)

Therefore, the total Q _BM of charge to ride the black matrix is as shown in the following equation.

_{Q BM = (C BM-TCE} + C BM-TCL) × V TC + C BM-TPE × V TP + (C BM-RCE + C BM-RCL) × V RC + C BM-RPE × V RP + (C BM-Ga + C _BM-Gb ) × V _G + (C _BM-Da + C _BM-Db ) × V _D (3)

When the whole screen is displayed in black, the numerator portion of the above formula includes a charge _{QBM (1)} on the same or the same side with respect to the transmissive pixel electrode and a charge _{QBM (} inverted or negative with respect to the transmissive pixel electrode _{). 2)} .

_{Q BM (1) = (C} BM-TCE + C BM-TCL) × V TC + C BM-TPE × V TP + (C BM-Da + C BM-Db) × V D + C BM-RPE × V RP ( write frame To 2n frames) (4)

_{Q BM (2) = (C} BM-RCE + C BM-RCL) × V RC + C BM-RPE × V RP (2n + 1 frame from the write _{frame) + (C BM-Ga +} C BM-Gb) × V G ... (5 )

In addition, potential V _BM of the black matrix is as shown in the following equation.

V _BM = _{Q BM / C BMTOTAL
= [(C BM-TCE +} C BM-TCL) × V TC + C BM-TPE × V TP + (C BM-RCE + C BM-RCL) × V RC + C BM-RPE × V RP + (C BM-Ga + C _{BM-Gb) × V G +} (C BM-Da + C BM-Db) × V D] / [C BM-TCE + C BM-TCL + C BM-TPE + C BM-RCE + C BM-RCL + C BM-RPE + C BM _-Ga + _{CBM -Gb} + _CBM-Da + _CBM-Db ] (6)

Here, since the scanning line and the data line in the display unit are covered and electrically shielded by the transmissive common electrode or the reflective common electrode, it may be considered that there is no influence of each black matrix. Also, the scanning lines and data lines in the peripheral part can be similarly covered by using the same conductive film as that of the transmissive common electrode, and the influence on the black matrix can be similarly eliminated. With such a structure, the terms _CBM-Da , _CBM-Db , _CBM-Ga , and _CBM-Gb are substantially eliminated, and the reflective common electrode, the reflective common electrode line, the transmissive common electrode, It is sufficient to consider the interaction between each of the transmissive common electrode lines and the black matrix.

In the liquid crystal display device, in the region where no voltage is applied between the common electrode and the pixel electrode, the influence of the potential of the black matrix becomes large, and the display quality greatly deteriorates due to light leakage in the black display state. As described above, when gate line inversion driving or dot inversion driving is used, black display is obtained when a voltage is applied only to the reflective region. Therefore, in order to reduce the potential difference between _VBM and _VTC , It is necessary to increase the contribution of _{QBM (1)} or reduce the contribution of _{QBM (2)} .

  Further, charge Q∝capacitance C × voltage V∝ε × S × V / d (ε is the relative dielectric constant of the constituent material between the black matrix and each electrode and wiring, and S is the black matrix and each electrode and wiring The overlapping area, d, is a relationship between the black matrix and the distance between each electrode and wiring.

  Therefore, the following method is effective for reducing the potential difference between the electrode in the transmission region and the black matrix.

(1) Since the capacitance changes in proportion to the area where the black matrix and each electrode and wiring overlap, in order to increase the contribution of _{QBM (1)} , _CBM-TCE , _CBM-TCL , C _{In order} to increase the electrode area for forming _BM-TPE , _CBM-Da , and _CBM-Db , or to reduce the contribution of _{QBM (2)} , _CBM-RCE , _CBM-RCL , and _{CBM The} electrode area for forming _-Ga and _{CBM -Gb} is reduced, or the black matrix is separated and shielded so that the potential of the transmission region is not affected.

(2) Since the charge changes in proportion to the voltage, in order to increase the contribution of Q _{BM (1)} , to increase V _TC or to reduce the contribution of Q _{BM (2)} , V _RC and V _G are lowered. That is, it is only necessary to increase the amplitude of the transmission common signal, decrease the amplitude of the reflection common signal, or increase the voltage when the gate signal is off.

(3) Since the capacitance is inversely proportional to the distance between the black matrix and each electrode and wiring, in order to increase the contribution of _{QBM (1)} , the black matrix, the transmissive common electrode, the transmissive pixel electrode, data In order to reduce the spacing between the lines, or to reduce the contribution of _{QBM (2)} , the spacing between the black matrix, the reflective common electrode, and the scanning lines is increased.

(4) Since the capacitance is proportional to the relative permittivity of the constituent material between the black matrix and each electrode and wiring, in order to increase the contribution of _{QBM (1)} , the black matrix and the transmissive common electrode, A low dielectric constant is interposed between the black matrix, the reflective common electrode, and the scanning line in order to sandwich a high dielectric constant member between the transmissive pixel electrode and the data line, or to reduce the contribution of _{QBM (2).} The member is sandwiched.

  By using these methods, the potential difference between the transmissive region electrode and the black matrix can be reduced. Preferably, the potential difference is made equal to or lower than the threshold at which the liquid crystal operates to suppress light leakage. Can do. Each method will be described below with reference to the drawings.

  First, a liquid crystal display device according to a first embodiment of the present invention will be described with reference to FIGS. 1A and 1B are plan views showing the structure of a transflective liquid crystal display device according to the present embodiment. FIG. 1A shows a structure excluding a reflector, and FIG. 1B shows a structure with a reflector and a black matrix added. ing. FIG. 2 is a cross-sectional view showing the structure of the transflective liquid crystal display device of this example. FIG. 2A is a cross-sectional view taken along line AA ′ of FIG. 1B, and FIG. Section (c) shows the structure of the section CC ′. 3 to 5 are diagrams showing another structure of the transflective liquid crystal display device of this embodiment, and FIG. 6 is a diagram showing the effect of this embodiment. 7 to 10 are diagrams for explaining inversion driving, and FIGS. 11 to 15 are diagrams showing types of liquid crystal display devices to which the structure of this embodiment is applied.

  As shown in FIGS. 1 and 2, the liquid crystal display device according to the present embodiment includes a first substrate (referred to here as a counter substrate 20) disposed on the viewing surface side, a TFT (Thin Film Transistor), and the like. A second substrate (referred to herein as TFT substrate 10) having an active element and having a transmissive region functioning as a transmissive liquid crystal display device and a reflective region functioning as a reflective liquid crystal display device, and between the two substrates. A liquid crystal layer 30 sandwiched between the first substrate, a first polarizing plate (not shown) disposed on the viewing surface side of the counter substrate 20, and a second polarizing plate disposed on the backlight source side of the TFT substrate 10 (see FIG. (Not shown).

  The TFT substrate 10 includes a plurality of scanning lines 12, data lines 13, and common electrode lines 5 arranged in a matrix on a transparent insulating substrate 11, and the common electrode line applies a reference potential to the transmissive region 3. The line 18a and the reflection common electrode line 18b for applying the reference potential to the reflection region 2 are provided. At the intersection of the scanning line 12 and the data line 13, a transmission TFT and a transmission pixel electrode 17a corresponding to the transmission region 3 of the pixel are provided. And a reflective TFT and a reflective pixel electrode 17b corresponding to the reflective region 2 of the pixel.

  A transmissive common electrode 18a 'is electrically connected to the transmissive common electrode line 18a, and a reflective common electrode 18b' is electrically connected to the reflective common electrode line 18b.

  The transmissive common electrode 18a ', the transmissive pixel electrode 17a, the reflective common electrode 18b', and the reflective pixel electrode 17b are usually formed of ITO (Indium Tin Oxide) or the like. The transmissive pixel electrode 17a and the transmissive common electrode 18a ′ are arranged in a stripe shape so that both electrodes are parallel to each other as shown in FIG. 1, and an electric field mainly composed of a component orthogonal to both electrodes parallel to the substrate surface. The reflection pixel electrode 17b and the reflection common electrode 18b ′ are arranged in a stripe shape so that both electrodes are parallel to each other, as shown in FIG. It is possible to generate an electric field (reflection) mainly composed of a component orthogonal to.

  As shown in FIGS. 1 and 2A, the reflection plate 15 is formed in the reflection region via the insulating film 15b below the reflection common electrode 18b 'and the reflection pixel electrode 17b.

  An alignment film (not shown) for controlling the liquid crystal alignment is formed on the TFT substrate 10 on the liquid crystal layer 30 side.

  In the counter substrate 20, a black matrix 22 and a color filter 23 are formed on a transparent insulating substrate 21.

  The black matrix 22 is formed by dispersing carbon particles or black pigment in a resin, and is disposed in a portion that shields light leakage of the display portion, for example, a portion that overlaps the scanning line 12 or the data line 13. Light leakage caused by the electric field between the electrodes generated between the reflective regions is shielded, and light leakage between wirings other than the display portion is suppressed.

  The distance between the TFT substrate 10 and the counter substrate 20, that is, the thickness of the liquid crystal layer 30 is set so that the phase difference is λ / 2 when a voltage is applied to display white in the transmissive region. In the region, the phase difference is set to λ / 4 when a voltage is applied to display black.

  The liquid crystal molecules of the liquid crystal layer 30 have a homogeneous orientation parallel between the substrates, the director direction is oriented in a direction inclined by 15 degrees from the stripe direction of the electrode, and an electric field formed between the common electrode and the pixel electrode. The direction can be changed.

  On the opposite side of the TFT substrate 10 and the counter substrate 20 from the liquid crystal layer 30, the polarizing plates are arranged so that the absorption axes are orthogonal to each other, and the initial director direction and the direction of the absorption axis of one of the polarizing plates coincide. Are arranged as follows.

  This embodiment is characterized by the positional relationship between the common electrode line or common electrode formed on the TFT substrate 10 and the black matrix 22 formed on the counter substrate 20. A film thickness, a manufacturing method, etc. are not specifically limited.

  Here, as described above, in the transflective liquid crystal display device, since black display and white display are reversed, it is necessary to drive by applying voltages having different phases to the transmissive region and the reflective region. When different voltages are applied, the potential of the black matrix 22 changes, and the potential difference between the transmissive common electrode line 18a, the transmissive common electrode 18a ′, the transmissive pixel electrode 17a, and the black matrix 22 increases.

  Therefore, in this embodiment, in order to solve this problem, an area where the transmissive common electrode line 18a, the transmissive common electrode 18a ', the transmissive pixel electrode 17a and the black matrix 22 overlap is increased.

Specifically, as shown in FIG. 1 and FIGS. 2B and 2C, a transmissive common electrode 18a ′ and a reflective common electrode 18b ′ are arranged on the data line 13, and the black matrix 22 has data. Since it is arranged so as to cover the line 13, the width of the black matrix 22 arranged on the transmissive common electrode 18a ′ is made wider than the width of the black matrix 22 arranged on the reflective common electrode 18b ′. Thereby, the electrode area for forming the capacitor C _BM-TCE between the transmissive common electrode 18 a ′ and the black matrix 22 is larger than the electrode area for forming the capacitor C _BM-RCE between the reflective common electrode 18 b ′ and the black matrix 22. And the contribution of the charge _{QBM (1)} on the same side or the same side to the transmissive common electrode 18a ′ can be increased.

  In this case, the width of the black matrix 22 disposed on the transmissive common electrode 18a ′ may be wider than that of the conventional structure shown in FIG. 26C, or may be disposed on the reflective common electrode 18b ′. The width of the black matrix 22 may be narrower than that of the conventional structure shown in FIG. When the width of the black matrix 22 arranged on the reflective common electrode 18b ′ is narrowed, there is a concern about light leakage from the side of the black matrix 22, but in this case, the reflective common electrode 18b ′ and the reflective pixel in the reflective region 2 are concerned. The electrode 17b is blackened by oxidizing the ITO, the reflected light is reduced by increasing the ITO film thickness and decreasing the ITO transmittance, or a metal having a lower reflectance than the reflector (for example, chromium or molybdenum) Metal film), preferably a low-reflective metal (for example, an oxide laminated film such as two-layer chromium Cr / CrO or two-layer nickel Ni / NiO) can suppress light leakage from the side of the black matrix. In addition, light leakage caused by performing liquid crystal alignment different between the reflective common electrode and the reflective pixel electrode can be suppressed at the same time. Can, it is possible to increase the contrast of reflection.

  In FIGS. 1 and 2, the width of the black matrix 22 disposed on the transmissive common electrode 18a ′ is widened or the width of the black matrix 22 disposed on the reflective common electrode 18b ′ is narrowed. As shown in FIG. 3, the same effect can be obtained even if the reflective common electrode 18b ′ on the data line 13 is narrowed, and the width of the transmissive common electrode 18a ′ on the data line 13 is shown in FIG. The same effect can be obtained even if the width is widened.

  1 to 4, the relationship between the electrodes of the display unit and the black matrix 22 is defined. However, the transmissive common electrode line 18a and the reflective common electrode line 18b are routed around the periphery of the display unit. Therefore, as shown in FIG. 5, the width of the transmissive common electrode line 18 (wiring connected to the non-inverting amplifier circuit, dark-colored wiring in the drawing) may be widened, or the reflective common electrode line 18b. The width of the wiring connected to the inverting amplifier circuit (light wiring in the figure) may be narrowed.

  The method for increasing the area where the transmissive common electrode line 18a, the transmissive common electrode 18a ′, the transmissive pixel electrode 17a and the black matrix 22 overlap is described above, but what is the area where the black matrix 22 is overlapped? In order to confirm this, as in the prior art, the sample in which the black matrix 22 having the same width is formed in the reflective region 2 and the transmissive region 3 is superimposed on the transmissive common electrode 18a and the black matrix 22 by any one of the above methods. A sample in which the area was changed relative to the overlapping area of the reflective common electrode 18b ′ and the black matrix 22 was prepared.

  Then, display is performed by performing gate line inversion driving in which the phase of the pixel potential and the common potential is inverted for each scanning line 12. In this case, as shown in FIGS. 7 and 8, the same signal (D) is supplied from each TFT to the transmissive pixel electrode 17a and the reflective pixel electrode 17b from the data line 13. Further, a transmission common signal (Tcom) that is inverted for each line is sent to the transmission common electrode line 18a, and a reflection common signal (Rcom) whose phase is inverted from that of the transmission common signal is supplied to the reflection common electrode line 18b. Is done.

  7 and 8, the amplitude of the reflection common signal (Rcom) is the same as that of the transmission common signal (Tcom), but it is the same depending on the interval between the common electrode and the pixel electrode and the thickness of the liquid crystal layer. It may be made different or different. Here, the amplitude of the transmission common signal (Tcom) is adjusted to 5.2 V, and the amplitude of the reflection common signal (Rcom) is also adjusted to be the same. The distance between the transmissive pixel electrode 17a and the transmissive common electrode 18a ′ is 8 μm, the distance between the reflective pixel electrode 17b and the reflective common electrode 18b ′ is 4 μm, and the thickness of the liquid crystal layer 30 in the transmissive region 3 is 3.2 μm. The thickness of the liquid crystal layer 30 in the reflective region 2 was set to 2.0 μm.

  When the gate line inversion driving is outlined, in FIG. 7A, in the line where G and D are High, the D signal is applied to the transmissive pixel electrode 17a and the reflective pixel electrode 17b of each pixel in the reflective region and the transmissive region. The potential is + 5V, but the transmission common signal (Tcom) is 0V and the reflection common signal (Rcom) is + 5V. Therefore, the potential difference between the transmission pixel electrode 17a and the transmission common electrode 18a ′ is + 5V, and the reflection pixel electrode 17b. And the reflection common electrode 18b ′ has a potential difference of 0V. In the line where G and D are Low, the potentials of the transmissive pixel electrode 17a and the reflective pixel electrode 17b are 0V, but Tcom is + 5V and Rcom is 0V. Therefore, the transmissive pixel electrode 17a and the transmissive common electrode 18a ′. Is + 5V, and the potential difference between the reflective pixel electrode 17b and the reflective common electrode 18b 'is 0V. As a result, an electric field is applied to the liquid crystal layer only in the transmission region, and the liquid crystal molecules rotate.

  In this state, in the liquid crystal display device in which both the reflective region 2 and the transmissive region 3 are driven in the IPS mode, as shown in FIGS. 11 and 12, in the reflective region (upper right side of FIG. 12), the first polarizing plate is formed in the liquid crystal layer. 90 ° direction (longitudinal) linearly polarized light that has passed through the incident light passes through the liquid crystal layer, is reflected by the reflecting plate, remains at 90 ° linearly polarized light, and passes through the liquid crystal layer again and enters the first polarizing plate. And pass through the first polarizing plate. On the other hand, in the transmission region (the upper left side of FIG. 12), the linearly polarized light in the horizontal direction that has passed through the second polarizing plate is incident on the liquid crystal layer, but the major axis direction of the liquid crystal layer in the liquid crystal layer changes due to voltage application, The laterally linearly polarized light incident on the liquid crystal layer becomes longitudinally linearly polarized light and enters the first polarizing plate and passes through the first polarizing plate. Accordingly, both the reflection area and the transmission area are displayed in white.

  In FIG. 7B, in the line where G is High and D is Low, the potentials of the transmissive pixel electrode 17a and the reflective pixel electrode 17b are 0V, but Tcom is 0V and Rcom is + 5V. The potential difference between the pixel electrode 17a and the transmissive common electrode 18a ′ is 0V, and the potential difference between the reflective pixel electrode 17b and the reflective common electrode 18b ′ is + 5V. In the line where G is Low and D is High, the potentials of the transmissive pixel electrode 17a and the reflective pixel electrode 17b are + 5V, but Tcom is + 5V and Rcom is 0V. Therefore, the transmissive pixel electrode 17a and the transmissive common electrode The potential difference from 18a ′ is 0V, and the potential difference between the reflective pixel electrode 17b and the reflective common electrode 18b ′ is + 5V. As a result, an electric field is applied to the liquid crystal layer only in the reflective region, and the liquid crystal molecules rotate.

  In this state, as shown in FIGS. 11 and 12, in the reflection region (the lower right side of FIG. 12), the 90 ° direction (vertical direction) linearly polarized light that has passed through the first polarizing plate is incident on the liquid crystal layer. Since the major axis direction of the liquid crystal layer in the liquid crystal layer is changed by applying a voltage, the longitudinally linearly polarized light incident on the liquid crystal layer enters the reflecting plate in a counterclockwise circularly polarized state. This counterclockwise circularly polarized light is reflected by the reflecting plate to become a counterclockwise circularly polarized state, passes through the liquid crystal layer again, becomes a linearly polarized light in the lateral direction (0 ° direction), and enters the first polarizing plate. . Since the polarization axis direction of the first polarizing plate is 90 °, the reflected light is not allowed to pass through. On the other hand, in the transmission region (lower left side of FIG. 12), the linearly polarized light in the horizontal direction that has passed through the second polarizing plate enters the liquid crystal layer, passes through the liquid crystal layer, and enters the first polarizing plate. Since the polarization axis direction of the first polarizing plate is 90 °, transmitted light is not allowed to pass through. Therefore, both the reflective area and the transmissive area are displayed in black.

  As described above, even if the same video signal is applied to the display of the transmissive region 3 and the reflective region 2, the same black display and white display can be performed in the reflective display and the transmissive display.

  Here, St1 is an area where the transmissive common electrode line 18a and the black matrix 22 are overlapped to face each other, St1 is an area where the transmissive common electrode 18a ′ and the black matrix 22 are oppositely overlapped, and St2 is a reflection common electrode line 18b. And Sr2 the area where the black matrix 22 and the black matrix 22 face each other, and Sr2 the area where the reflective common electrode 18b 'and the black matrix 22 face each other. Is called the area transmission ratio α):

  Area transmission ratio α = (St1 + St2) / (St1 + St2 + Sr1 + Sr2) (7)

  Then, the overlapping area of the transmissive common electrode 18a ′ and the transmissive common electrode line 18a and the black matrix 22 is set to the overlapping area of the reflective common electrode 18b ′ and the reflective common electrode line 18b and the black matrix 22 by any one of the methods described above. The contrast ratio was measured using samples that were relatively varied so that α was 54%, 64%, 72%, and 100%. Here, α = 100% means a state where a transmission common signal (Tcom) is applied to the reflective common electrode line 18b.

  As a result, as shown in FIG. 6, the contrast ratio is 140: 1 for the α = 54% sample, 180: 1 for the α = 64% sample, 450: 1 for the α = 72% sample, and α = 100%. In this sample, it changed to 450: 1.

  Further, when the waveform was examined with an oscilloscope, the potential of the black matrix 22 (the fine broken line in the figure) of the sample with α = 54% is A line (transmission common signal is Low, reflected by the influence of the scanning line signal. The black signal is an intermediate potential where the potential does not change in both the common signal is a high line and the B line that is the next line of A (the transmission common signal is high and the reflection common signal is low). It is considered that the contrast ratio was lowered because the potential of 22 produced a large potential difference with the transmission common signal in both A and B. In addition, in the sample with α = 72%, the potential of the black matrix 22 is close to the transmission region in both the phase A line and the B line due to the influence of the scanning line signal. As a result, the liquid crystal does not operate between the black matrix and the transmissive common electrode and the transmissive pixel electrode, and it is considered that the contrast ratio is improved because no light leakage occurs. In this experiment, the shield of the scanning line is not partly. Therefore, the time during which the voltage (−12 V) that is turned off is flowing is longer than the time during which the voltage (+12 V) that turns on the TFT is flowing. Is longer and therefore shifts to the negative side as a whole. That is, when α = 54%, the A line is a common transmission signal, whereas the B line is a reflection common signal, which causes light leakage due to the B line. It is necessary to shield the scanning line.

  Here, the potential of the black matrix can be measured using an oscilloscope in a state in which the counter substrate is shaved to expose the black matrix and in direct contact with a conductive material such as solder. The reflection common signal and the transmission common signal can be measured with an oscilloscope by shaving the film covering the reflection common signal line and the transmission common signal line of the TFT substrate in the same manner as measuring the black matrix potential. If it is supplied from outside, it may be measured.

  Further, when the black display pixels are observed, when α = 54%, the periphery of the transmissive common electrode 18a ′ is shining, whereas when α = 72% and α = 100%. There was no light leakage.

  From the above results, if the area where the common electrode line or the common electrode overlaps with the black matrix 22 is adjusted so that the area transmission ratio α> 72%, the gap between the transmissive pixel electrode 17a ′ and the transmissive common signal is adjusted. Even when black display with no potential difference is performed, the potential difference between the black matrix 22 and the transmission common signal becomes small, so that rotation of the director is suppressed and light leakage can be suppressed.

  Here, when the capacitance is calculated from the area formed by St1, St2, Sr1, and Sr2, and Ct1, Ct2, Cr1, and CCr2, respectively, the capacitance transmission ratio αc is expressed by the following equation.

Capacity transmission ratio α _C = (Ct1 + Ct2) / (Ct1 + Ct2 + Cr1 + Cr2) (8)

The levels of α _S = 54%, 64%, 72%, and 100% are α _C = 50%, 60%, 73%, and 100%, respectively. Since the transmission common signal and the reflection common signal are applied with signals having the same amplitude, the black matrix potential can be found to be biased toward the black matrix potential as it is with α _C. When α _C = 50%, the black matrix potential becomes an intermediate potential between the transmission common signal and the reflection common signal (lower left in FIG. 6), and as the capacitance transmission ratio increases, the black matrix potential approaches the transmission potential. Thus, it can be seen that the potential difference between the transmissive common electrode and the black matrix is reduced, and light leakage is reduced.

  In the above embodiment, the case where the transflective liquid crystal display device is operated by the gate line inversion driving in which the phase of the pixel potential and the common potential is inverted for each scanning line 12 is shown. The same effect can be obtained even when the pixel signal is applied and the common signal is driven by applying the same signal to both the reflective region and the transmissive region and driven by dot inversion driving as shown in FIGS. The example in the figure shows a method in which the same data lines are used for the transmissive region and the reflective region, gate lines are prepared in the respective regions, and different signals are applied in one line. Other methods may be used as long as different pixel signals are applied.

  In addition, the present invention is not limited to the liquid crystal display device in which both the reflective region 2 and the transmissive region 3 are driven in the IPS mode, and as shown in FIG. 15, both or one of the reflective region 2 and the excess region 3 is driven in the FFS mode. The present invention can be similarly applied to the liquid crystal display device, and as shown in FIGS. 13 and 14, the reflective common electrode 18 b ′ is formed on the counter substrate 20, and the reflective pixel electrode 17 b is formed on the TFT substrate 10. In addition, the present invention can be similarly applied to a liquid crystal display device driven in an ECB (Electrically Controlled Birefringence) mode in which the birefringence of the liquid crystal 30 is controlled by an electric field between the TFT substrate 10 and the counter substrate 20.

  FIGS. 13 and 14 show a method in which the liquid crystal 30 in the reflective region 2 is homogeneously aligned and a retardation plate is formed in the reflective region 2 for display, but a VA (Vertical Alignment) method perpendicular to the substrate is used. Even if it is used, the same display can be achieved even in the state of normally black and normally white by inversion driving.

  Here, a configuration is adopted in which normally black is displayed in the transmission region and normally white is displayed in the reflection region. For example, when the IPS method is used in both the transmission region and the reflection region, the angle of the polarizing plate is set to 45. By rotating it, the transmission area can be normally white and the reflection area can be normally black.

  Next, a liquid crystal display device according to a second embodiment of the present invention will be described with reference to FIGS. 16 and 17 are plan views showing the structure of the transflective liquid crystal display device of this embodiment. FIG. 18 is a diagram showing the contrast measured when the amplitude of the reflected common signal is changed.

  In the first embodiment described above, the influence of the transmission common signal is increased by increasing the overlapping area of the transmission common electrode 18a ′ and the black matrix 22, but the same effect can be obtained by reducing the influence of the reflection common signal. The effect can be expected. In this embodiment, like the first embodiment, the distance between the reflective common electrode and the reflective pixel electrode is halved to 4 μm with respect to the thickness of the liquid crystal layer and the distance between the transparent common electrode and the transmissive pixel electrode of 8 μm. However, when the number of electrodes increases, there is a problem that the liquid crystal on the electrodes does not rotate relative to the substrate plane direction than the liquid crystal between the electrodes, so that it always shines. Therefore, the electrode area can be reduced by increasing the reflective electrode interval from 4 μm to 6 μm. However, by increasing the electrode interval, it is necessary to increase the voltage applied between the electrodes, and it is necessary to increase the reflected common signal to 8V.

  First, in order to confirm the influence of the reflection common signal, the change in contrast when the voltage applied to the reflection common electrode 18b 'was changed was measured. The result is shown in FIG. From FIG. 18, as the amplitude of the reflected common signal increases, the brightness of white display decreases, the brightness of black display increases, and the contrast decreases. When the voltage in each state is checked with an oscilloscope, if the amplitude of the reflected common signal is 0 V, the potential of the black matrix 22 follows the transmitted common signal, but both the reflected common signal and the transmitted common signal have the same amplitude. When the phase is 5.2 V and the phase is opposite, the value is almost constant, and when the amplitude of the reflected common signal becomes 8 V, the potential of the black matrix 22 follows the reflected common signal. Therefore, when the amplitude of the reflection common signal increases, the potential of the black matrix 22 is pulled by the reflection common signal, and as a result, the potential difference between the transmission common signal and the black matrix 22 having the opposite phase to the reflection common signal increases. It is considered that light leakage occurs and the contrast decreases.

  Therefore, in this embodiment, in order to suppress the potential difference between the transmissive common signal and the black matrix 22, for example, as shown in FIG. 16, the black matrix 22 in the reflective region 2 and the black in the transmissive region 3 are displayed in the display unit. The matrix 22 is electrically separated. Further, as shown in FIG. 17, in the periphery of the display unit, the black matrix 22 on the transmissive common electrode line 18a and the black matrix 22 on the reflective common electrode 18b are electrically separated by forming a slit in a pattern. Adopted structure. Also, as shown in FIG. 17, among the black matrix 22 that forms the outer and peripheral portions of the display section, the black matrix on the reflective common electrode line 18b is the same as the black matrix 22 in the display section, and a slit is formed in the pattern. Thus, it is possible to adopt a structure in which the black matrix 22 is electrically separated, or the black matrix 22 can be electrically separated by forming a slit in a pattern between the display portion and the peripheral portion.

  By separating the black matrix 22 in this way, the potential of the black matrix 22 can follow the transmission common signal regardless of the amplitude of the reflection common signal, and as a result, the transmission common electrode 18a ′ or the transmission common electrode 18a. Leakage due to a potential difference between the black matrix 22 and the black matrix 22 can be suppressed, and the black matrix formed in the transmissive region is electrically separated by forming a slit between the black matrix formed in the reflective region. Thus, a contrast of 450: 1 could be realized.

In the structure of FIG. 16, since the scanning line 12 is formed in the region corresponding to the portion (slit portion) from which the black matrix 22 is separated, there is no fear that the transmitted light leaks, and this portion is formed by a reflector. The same effect can be obtained even if the structure is covered. Further, if the scanning line 12 is formed of a light shielding member, light leakage due to reflected light does not occur. Here, it has been described that the influence of _CBM-RCE can be excluded from the potential of the black matrix that affects the transmission region by adopting a structure that is separated by the display unit. By electrically separating it from the black matrix connected to, the influence of _CBM-RCL can be excluded, and the influence of the transparent common signal becomes relatively large.

  Next, a liquid crystal display device according to a third embodiment of the present invention is described with reference to FIG. FIG. 19 is a plan view showing the structure of the transflective liquid crystal display device of this example.

  In the second embodiment, the black matrix 22 is separated so that the black matrix 22 is not affected by the reflection common signal. However, the reflection common electrode 18b ′ or the reflection common electrode line 18b is made of a conductive film. The influence of the reflected common signal can also be suppressed by shielding by applying another potential.

  For example, as shown in FIG. 19, the reflection common electrode line 18b (wiring connected to the inverting amplification circuit in the figure) at the periphery of the TFT substrate 10 of the liquid crystal display device is formed of the same metal as the gate line, and on that A shield is formed of the same ITO as the pixel electrode and the common electrode, and a transmission common signal is given by connecting to the transmission common electrode line through the contact hole. In this way, the area where the reflective common electrode line and the black matrix overlap can be changed to a potential in phase with the transmissive common electrode line, and the black matrix potential increases the contribution of the transmissive common signal. be able to.

  The reflective common electrode line is the same metal as the gate line, and the shield is formed from the same metal as the pixel electrode and the common electrode, but a conductive layer is formed between the reflective common electrode line and the black matrix to Since an electric potential may be applied, it may be formed of another conductive layer, or a member for shielding may be newly added. Further, the shield is not limited to the TFT substrate, but may be formed on the counter substrate side, and the transmission common signal may be given in the same manner.

  Next, a liquid crystal display device according to a fourth embodiment (reference invention) of the present invention will be described with reference to FIGS. 20 and 21 are a plan view and a cross-sectional view of the connection portion showing the structure of the transflective liquid crystal display device of this embodiment.

  In the first to third embodiments described above, the method has been described which is easily influenced by the transmission common signal or less influenced by the reflection common signal. However, by applying the transmission common signal to the black matrix 22, The potential difference between the transmissive common electrode and the black matrix can be eliminated.

  In this embodiment, as shown in FIG. 20, a contact electrode is formed on the transmissive common electrode line 18a of the TFT substrate 10 in the peripheral portion (for example, a broken line portion in the figure), and the conductive paste or the surface is subjected to the conductive treatment. The potential can be applied by connecting the contact electrode and the black matrix 22 using the performed particles or the like. In addition, as shown in FIG. 21, there is a method in which a circuit for supplying a signal having the same phase as the transmission common signal to the black matrix is prepared separately from the transmission common electrode line 18a and connected in the same manner as in FIG. In such a method, since a signal different from the transmission common signal can be applied, for example, another signal can be given by display.

  Here, the black matrix 22 may be a material in which carbon black is dispersed in a resin. In order to sufficiently apply a potential, it is necessary to make a large contact area. The contact hole can be made small by using a metal such as Cr or a metal oxide laminated on the black matrix.

  In addition, the connection structure and connection position of the transmissive common electrode line 18a or the black matrix electrode line and the black matrix 22 are not limited to the configuration shown in the drawing.

  Next, a liquid crystal display device according to a fifth embodiment of the present invention is described with reference to FIGS. 22 to 25 are cross-sectional views showing the structure of the transflective liquid crystal display device of this embodiment.

  In the first to fourth embodiments described above, the shape and structure of the common electrode and the black matrix 22 have been described. However, the same effect can be obtained by changing the distance between the common electrode and the black matrix 22 and the dielectric constant. Can do.

For example, as shown in FIG. 22, a step film is formed on the counter substrate side without forming a step film for adjusting the thickness of the liquid crystal layer between the passivation film and the reflective film on the data line. Can do. Here, the passivation film can also serve as the uneven film. With such a configuration, the distance between the black matrix, the reflective common electrode, and the reflective pixel electrode can be increased even if the thickness of the reflective liquid crystal layer is made thinner than that of the transmission, and the capacitance C formed therebetween is increased. _BM-RCE and _CBM-RPE can be reduced. If a structure having a dielectric constant lower than that of liquid crystal is employed, _CBM-RCE and _CBM-RPE can be further reduced. By adopting such a structure, even when the area of the reflection region is the same as that of the first embodiment, the potential of the black matrix can be controlled without unnecessarily reducing the black matrix 22 and the contrast. Rises.

Further, as shown in FIG. 23, the overcoat laminated on the black matrix and the color filter is made of different materials for the transmission region and the reflection region, and the reflection region overcoat has a dielectric constant higher than that of the transmission region overcoat. By adopting a low material, CBM-RCE and CBM-RPE can be made small. As shown in Fig. 24, the color filter is made of different materials for the reflective area and the reflective area. C _BM-RCE and C _BM-RPE can also be reduced by adopting a material having a dielectric constant lower than that of the color filter in the transmission region.

The low dielectric constant layer is formed between the reflective common electrode line and the scanning line and the black matrix, and the capacitances C _BM-RCL and C _BM-Ga between the reflective common electrode line and the scanning line and the black matrix are the same. Can be made smaller. For example, as shown in FIG. 25, it can be realized by placing a structure having a lower dielectric constant than the liquid crystal on the reflective common electrode line and the scanning line of the TFT substrate. This structure may be formed by the insulating film 15b or the step film, or may be newly created. Here, an example in which the TFT substrate is formed on the TFT substrate side is shown, but the same effect can be obtained by forming it on the counter substrate.

  In addition, the structure of each said Example may be applied separately, and may combine these arbitrarily. In addition, the present invention is not limited to the description of the above embodiment, and the common electrode in the normally black region and the potential difference formed between the pixel electrode and the black matrix are the common electrode in the normally white region. In addition, any structure may be used as long as one of the potential differences formed between the pixel electrode and the black matrix is smaller than the larger one.

  The present invention is applicable to a liquid crystal display device having a normally black region and a normally white region.

It is a top view which shows the structure of the transflective liquid crystal display device which concerns on 1st Example of this invention, (a) is a structure except a reflecting plate, (b) is a structure which added the reflecting plate and the black matrix. Is shown. It is sectional drawing which shows the structure of the transflective liquid crystal display device which concerns on 1st Example of this invention, (a) is the AA 'cross section of FIG.1 (b), (b) is BB'. Section (c) shows the structure of the section CC ′. 1 is a cross-sectional view showing the structure of a transflective liquid crystal display device according to a first embodiment of the present invention. 1 is a cross-sectional view showing the structure of a transflective liquid crystal display device according to a first embodiment of the present invention. 1 is a plan view showing a structure of a transflective liquid crystal display device according to a first embodiment of the present invention. It is a figure which shows the effect of the 1st Example of this invention, and has shown the correlation with area transmission ratio and contrast. It is a figure explaining gate line inversion drive. It is a figure explaining gate line inversion drive. It is a figure explaining dot inversion drive. It is a figure explaining dot inversion drive. It is sectional drawing which shows the structure of the transflective liquid crystal display device of IPS (reflection) / IPS (transmission). It is a figure which shows operation | movement of the transflective liquid crystal display device of IPS (reflection) / IPS (transmission). It is sectional drawing which shows the structure of the transflective liquid crystal display device of ECB (reflection) / IPS (transmission). It is a figure which shows operation | movement of the transflective liquid crystal display device of ECB (reflection) / IPS (transmission). It is sectional drawing which shows the structure of the transflective liquid crystal display device of FFS (reflection) / FFS (transmission). It is a top view which shows the structure of the transflective liquid crystal display device based on the 2nd Example of this invention. It is a top view which shows the structure of the transflective liquid crystal display device based on the 2nd Example of this invention. It is a figure which shows the relationship between the amplitude of a reflection common signal, and contrast. It is a top view which shows the structure of the transflective liquid crystal display device based on the 3rd Example of this invention. It is the top view which shows the structure of the transflective liquid crystal display device which concerns on the 4th Example of this invention, and sectional drawing of a connection part. It is the top view which shows the structure of the transflective liquid crystal display device which concerns on the 4th Example of this invention, and sectional drawing of a connection part. It is sectional drawing which shows the structure of the transflective liquid crystal display device based on the 5th Example of this invention. It is sectional drawing which shows the structure of the transflective liquid crystal display device based on the 5th Example of this invention. It is sectional drawing which shows the structure of the transflective liquid crystal display device based on the 5th Example of this invention. It is sectional drawing which shows the structure of the transflective liquid crystal display device based on the 5th Example of this invention. It is a top view which shows the structure of the conventional transflective liquid crystal display device, (a) is a structure except a reflecting plate, (b) is a structure where a reflecting plate is added, (c) is a structure where a black matrix is added. Is shown. It is sectional drawing which shows the structure of the conventional transflective liquid crystal display device, (a) is AA 'cross section of FIG.1 (b), (b) is BB' cross section, (c) is C The structure of the -C 'cross section is shown. It is a top view which shows the connection structure of the wiring of the conventional transflective liquid crystal display device. It is a figure which shows the waveform of a transmission common signal and a reflection common signal. It is a figure which shows the electric potential relationship of a transmissive common signal, a reflective common signal, and a black matrix. It is a figure which shows the electric potential and capacity | capacitance in the display part of a transflective liquid crystal display device. It is a figure which shows the electric potential and capacity | capacitance in the peripheral part of a transflective liquid crystal display device.

2 Reflection area 3 Transmission area 10 TFT substrate 11 Transparent insulating substrate 12 Scan line 13 Data line 14a, 14b TFT
15a Step / Uneven film 15b Insulating film 16 Reflector 17a Transparent pixel electrode 17b Reflective pixel electrode 18a Transparent common electrode line 18a 'Transparent common electrode 18b Reflective common electrode line 18b' Reflective common electrode 20 Counter substrate 21 Transparent insulating substrate 22 Black matrix 23 Color filter 24 Low ε layer 30 Liquid crystal layer

Claims (1)

In a liquid crystal display device comprising: one substrate on which switching elements are arranged in a matrix; the other substrate on which a black matrix made of a conductive material is formed; and a liquid crystal layer sandwiched between the two substrates.
The liquid crystal display device has a first region for normally black display and a second region for normally white display.
A first common electrode for supplying a first common signal to the first pixel electrode, the first common electrode, and the first common electrode electrically connected to the switching element is provided on the one substrate in the first region. Have a line,
The one substrate or the other substrate of the second region has a second common electrode,
The one substrate in the second region has a second pixel electrode electrically connected to the switching element and a second common electrode line for supplying a second common signal to the second common electrode. And
A liquid crystal display device, wherein a conductive film supplied with a potential different from that of the second common electrode line is formed between the second common electrode line and the black matrix in a peripheral portion of the display region.

Images